A brief description about large-\(N_c\)  chiral perturbation theory can be found in Ref. [1]}, so only a few aspects will be highlighted here. The starting point is the fact that in the large-\(N_c\)  limit, the baryon magnetic moments have the same kinematic properties as the baryon axial couplings so they can be expressed in terms of the very same operators [2]}. Since much of the work has already been advanced in Refs. [3]}, [4]}, [1]}, some partial results presented in these references will be borrowed for the purposes of the present analysis.
